The invention relates to an X-ray analysis apparatus comprising an X-ray source, a sample holder and an X-ray detector with a pulse counting amplifier being controlled by a correction voltage which is provided by a pulse amplitude shift comparison circuit as a measure of and in response to the occurrence of pulse amplitude shifts.
Such an apparatus is known in the form of an X-ray fluorescence spectrometer from GB 2 000 862. In such apparatus, pulse amplitude shifts may lead to the ocurrence of measurement errors which will adversely affect the accuracy of the analysis. Such pulse amplitude shifts are mainly due to variations in the natural amplification of the X-ray gas ionisation detector used, but can also result from thermal drift.
The invention has for its object to provide an automatic correction circuitry for such pulse amplitude shifts. According to the invention, an X-ray analysis apparatus of the kind mentioned in the opening paragraph is therefore characterized in that the pulse amplitude shift comparison circuit is provided with three parallel-connected amplitude discriminators, two of which, corresponding to a high and an intermediate amplitude discriminators, are connected to a high pass-range window circuit and two of which, corresponding to the intermediate and a low amplitude discriminators, are connected to a low pass-range window, both windows being connected to a comparator, which is provided with a memory, a control circuit connected to the comparator having a feed-back connection to the pulse amplifier.
When use is made of such a correction circuitry and the amplification of the pulse amplifier is readjusted by a correction voltage related to the extent of the pulse amplitude shift, in apparatus according to the invention, the pulses to be measured are restored to their correct value and can be measured more accurately or on the other hand variations in the natural amplification of the gas ionisation detector are substantially reduced.
In a preferred embodiment to each window circuit a rate meter is added, each of these rate meters converting the count rate in the corresponding channel into an analogue voltage.
In the comparator, these analogue voltages are compared with each other. When the voltages are unequal, a voltage variation is produced which as a control signal for the control part of an output voltage thereof is fed back to the controllable amplifier, as a result of which the amplification thereof is readjusted. By this control, the pulse peak is shifted back to a position fixed therefor.
An embodiment according to the invention will now be described with reference to the drawing. In the drawing:
An X-ray analysis apparatus shown in Figure 1 comprises an X-ray source 1, a sample holder 2, collimators 3 and 4, an analysing crystal 5 and a detector 6. An X-ray beam 7 strikes a test sample 8 and is there reflected in part. A reflected X-ray beam 9 incident via the collimator 3, on a surface 10 of the analysing crystal 5, after which a beam 11 reflected therefrom reaches the detector 6 via the collimator 4. A drive motor 4 acting via a transmission gear 15, causes the analysing crystal to rotate about an axis at right angles to the plane of the drawing. The motor 14 acting via a transmission gear 16, causes a rotation of the detector which matches the rotation of the crystal, likewise about an axis at right angles to the plane of the drawing. Due to this rotation, the detector is moved along an arc of a circle 17. The detector comprises, for example, a gas-filled detection cell, and measurement pulses which are generated therein by incident radiation quanta by ionisation, are applied to a pulse amplifier, which comprises a preamplifier 20 and a main amplifier 21. According to the invention, the amplifier has added to it a pulse shift correction circuit 22 to which is connected a recording device 23. Moreover, the preamplifier has connected to it a circuit element 26 which is connected to a reference voltage element 25 and in which by the adjustment of the apparatus given values for, for example the crystal type, the order of reflection, sine 8 and the sensitivity adjustment, are formed.
Figure 2 shows a more elaborate block circuit diagram of the detector reading system indicated in Figure 1 within a frame of dotted lines. For the sake of clarity, the amplifier 21 is subdivided into an adjustable amplifier 30 and a fixed amplifier31. The amplifier has connected to it in parallel arrangement three amplitude discriminators, i.e. a high threshold discriminator 32, an intermediate threshold discriminator 33 and a low threshold discriminator 34. Pulses accepted by the high threshold discriminator 32 are applied to an upper pass-range window circuit 35. Pulses accepted by the low threshold discriminator are passed on to a lower pass-range window circuit 36, while pulses accepted by the interemediate threshold discriminator are applied to both window circuits. The lower pass-range window circuit passes on only these pulses lying in an amplitude range between a lowthreshold level LL and an intermediate threshold level ML, whereas the upper pass-range window circuit passes on only those pulses lying between the intermediate threshold ML and a high threshold level HL. This is outlined in Figure 3, in which the number of pulses N is represented as a function of the pulse energy E. The amplitude pass-range window circuits further include rate meters 37 and 38, respectively. The rate meters form from the sequences of pulses passed by the respective window circuits, analogue voltage signals which are applied to a comparator circuit 39. In the comparator 39, the two voltage signals are compared with each other. When the two signals are unequal, a signal is formed which is a function of the occurring difference and this signal is applied to a control circuit 40. The amplification of the measurement pulses is thus adapted so that the centre ML of the pulse distribution is shifted to a fixed position corresponding to the intermediate threshold level set by the intermediate threshold discriminator 33. Thus, by means of the feedback mechanism, an active form of amplification correction is achieved which results in the intermediate value of the pulse distribution being maintained at a point which is fixed but adjustable. When due to a pulse amplitude shift in the detector, for example in a form of gas-filled counting tube, the amplification decreases, this decrease will be compensated for in the amplifier so that the overall amplification will remain constant. The advantage of such an active control correction is that - irrespective of the type of counting tube or of the high voltage used - it invariably compensates to the optimum. The measured signals can be displayed and recorded on a display device 41.